Differential-Equations Β· Unit 4 Β· Video 4 Β· Interactive Practice

Homogeneous Equations yβ€²=F(y/x)y' = F(y/x): Unchanged by Zoom, Solved by y=zxy = zx

IKey Formulas

FormulaNameWhat it says
yβ€²=F ⁣(yx)y' = F\!\left(\dfrac{y}{x}\right)Homogeneous equationEvery xx and yy on the right sits inside the one combination y/xy/x; not the "homogeneous linear" equation yβ€²+p(x)y=0y' + p(x)y = 0, which shares only the name
dy1dx1=F ⁣(y1x1)\dfrac{dy_1}{dx_1} = F\!\left(\dfrac{y_1}{x_1}\right)Zoom testAfter the zoom x=ax1x = ax_1, y=ay1y = ay_1 with a>0a > 0, the same equation in new names
y=zxβ€…β€Šβ‡’β€…β€Šyβ€²=zβ€²x+zy = zx \;\Rightarrow\; y' = z'x + zInverse substitutionThe product rule gives yβ€²y' in zz, zβ€²z' and xx alone
dzF(z)βˆ’z=dxx\dfrac{dz}{F(z) - z} = \dfrac{dx}{x}Separated formIntegrate, then put back z=y/xz = y/x; each line y=z0xy = z_0 x with F(z0)=z0F(z_0) = z_0 is a solution the division loses

Key Insight: The equation contains yβ€²y', so write the old variable in terms of the new one: y=zxy = zx hands over yβ€²=zβ€²x+zy' = z'x + z at once. The direct form z=y/xz = y/x gives zβ€²=xyβ€²βˆ’yx2z' = \dfrac{xy' - y}{x^2}, still in the old variables; it reaches the same xzβ€²=F(z)βˆ’zx z' = F(z) - z only after yβ€²=F(z)y' = F(z) and y=zxy = zx are put in.

IIInvariant Under Zoom

Zoom slides each point along its ray from the origin, where y/xy/x is fixed, so F(y/x)F(y/x) cannot change.

For x<0x < 0, x2=βˆ’x\sqrt{x^2} = -x turns the second example into yβ€²=βˆ’1+(y/x)2y' = -\sqrt{1 + (y/x)^2}: still a function of y/xy/x, so it passes the zoom test there too.

IIIThe Four Steps on the First Example

The method solves yβ€²=x2yx3+y3y' = \dfrac{x^2 y}{x^3 + y^3}, and the division in step 3 loses the line y=0y = 0.

Step 1 β€” Recognise
yβ€²=x2yx3+y3=y/x1+(y/x)3y' = \frac{x^2 y}{x^3 + y^3} = \frac{y/x}{1 + (y/x)^3}
F(z)=z1+z3F(z) = \frac{z}{1 + z^3}
Step 2 β€” Substitute
y=zx,yβ€²=zβ€²x+zy = zx, \quad y' = z'x + z
zβ€²x+z=z1+z3z'x + z = \frac{z}{1 + z^3}
x dzdx=z1+z3βˆ’z=βˆ’z41+z3x\,\frac{dz}{dx} = \frac{z}{1 + z^3} - z = -\frac{z^4}{1 + z^3}
Step 3 β€” Separate and integrate
1+z3z4 dz=βˆ’dxx(zβ‰ 0)\frac{1 + z^3}{z^4}\,dz = -\frac{dx}{x} \qquad (z \ne 0)
βˆ’13z3+ln⁑∣z∣=βˆ’ln⁑∣x∣+c-\frac{1}{3z^3} + \ln|z| = -\ln|x| + c
Step 4 β€” Put back
z=yx:ln⁑∣z∣+ln⁑∣x∣=ln⁑∣y∣z = \frac{y}{x}: \quad \ln|z| + \ln|x| = \ln|y|
ln⁑∣y∣=x33y3+c\ln|y| = \frac{x^3}{3y^3} + c
x3=3y3(ln⁑∣y∣+C),C=βˆ’cx^3 = 3y^3\big(\ln|y| + C\big), \quad C = -c

IVQuiz Questions

Problem 1 Β· The Zoom Test

Given: the zoom x=ax1x = ax_1, y=ay1y = ay_1 with a>0a > 0. Which equation comes back unchanged, and so is homogeneous?

βœ… Correct! Top and bottom both have degree 2, so the zoom multiplies each by a2a^2 and the factors cancel: dy1dx1=x12+y12x1y1\dfrac{dy_1}{dx_1} = \dfrac{x_1^2 + y_1^2}{x_1 y_1}.
❌ Not quite. The y/xy/x term survives the zoom, but y2y^2 becomes a2y12a^2 y_1^2, so the zoomed equation dy1dx1=y1x1βˆ’a2y12\dfrac{dy_1}{dx_1} = \dfrac{y_1}{x_1} - a^2 y_1^2 is a different one. Containing y/xy/x is not enough.
❌ Not quite. The numerator has degree 1 and the denominator degree 2, so the zoom leaves a factor aa2=1a\dfrac{a}{a^2} = \dfrac{1}{a}: dy1dx1=1aβ‹…x1+y1x12\dfrac{dy_1}{dx_1} = \dfrac{1}{a}\cdot\dfrac{x_1 + y_1}{x_1^2}.
❌ Not quite. The constant 11 does not scale: dy1dx1=ay1+1ax1=y1x1+1ax1\dfrac{dy_1}{dx_1} = \dfrac{ay_1 + 1}{ax_1} = \dfrac{y_1}{x_1} + \dfrac{1}{ax_1}, which still depends on aa.
Show solution

Under the zoom dydx=a dy1a dx1=dy1dx1\dfrac{dy}{dx} = \dfrac{a\,dy_1}{a\,dx_1} = \dfrac{dy_1}{dx_1}, so only the right-hand side can change. Substitute x=ax1x = ax_1, y=ay1y = ay_1 into (c):

(ax1)2+(ay1)2(ax1)(ay1)=a2(x12+y12)a2x1y1=x12+y12x1y1\frac{(ax_1)^2 + (ay_1)^2}{(ax_1)(ay_1)} = \frac{a^2(x_1^2 + y_1^2)}{a^2 x_1 y_1} = \frac{x_1^2 + y_1^2}{x_1 y_1}

The equation comes back identical. Dividing top and bottom by x2x^2 shows its FF: yβ€²=1+(y/x)2y/xy' = \dfrac{1 + (y/x)^2}{y/x}, so F(z)=1+z2zF(z) = \dfrac{1 + z^2}{z}.

The other three pick up aa: (a) becomes y1x1βˆ’a2y12\dfrac{y_1}{x_1} - a^2 y_1^2, (b) becomes 1aβ‹…x1+y1x12\dfrac{1}{a}\cdot\dfrac{x_1 + y_1}{x_1^2}, and (d) becomes y1x1+1ax1\dfrac{y_1}{x_1} + \dfrac{1}{ax_1}.

Problem 2 Β· Substituting for yβ€²

Given: xyβ€²=x2+y2x y' = \sqrt{x^2 + y^2} with x>0x > 0, that is yβ€²=1+(y/x)2y' = \sqrt{1 + (y/x)^2}. Which separated equation does the substitution y=zxy = zx produce?

βœ… Correct! yβ€²=zβ€²x+zy' = z'x + z turns the equation into x dzdx=1+z2βˆ’zx\,\dfrac{dz}{dx} = \sqrt{1 + z^2} - z, whose right side depends on zz alone.
❌ Not quite. This drops the +z+z from yβ€²=zβ€²x+zy' = z'x + z and treats yβ€²y' as zβ€²xz'x. The product rule gives both terms, and moving that zz to the right is what makes the denominator F(z)βˆ’zF(z) - z.
❌ Not quite. This uses yβ€²=zβ€²+zy' = z' + z. The derivative of zxzx is zβ€²x+zz'x + z, and the xx multiplying zβ€²z' is what becomes dxx\dfrac{dx}{x} on the right.
❌ Not quite. Moving zz across the equals sign subtracts it: xzβ€²=1+z2βˆ’zx z' = \sqrt{1 + z^2} - z, not 1+z2+z\sqrt{1 + z^2} + z.
Show solution

Substitute both pieces, yβ€²=zβ€²x+zy' = z'x + z on the left and y/x=zy/x = z on the right:

zβ€²x+z=1+z2β€…β€ŠβŸΉβ€…β€Šx dzdx=1+z2βˆ’zz'x + z = \sqrt{1 + z^2} \;\Longrightarrow\; x\,\frac{dz}{dx} = \sqrt{1 + z^2} - z dz1+z2βˆ’z=dxx\frac{dz}{\sqrt{1 + z^2} - z} = \frac{dx}{x}

No line is lost by the division: 1+z2>∣z∣β‰₯z\sqrt{1 + z^2} > |z| \ge z, so F(z)βˆ’zF(z) - z is never zero. Since (1+z2βˆ’z)(1+z2+z)=1\big(\sqrt{1 + z^2} - z\big)\big(\sqrt{1 + z^2} + z\big) = 1, the left side is (1+z2+z) dz\big(\sqrt{1 + z^2} + z\big)\,dz, and integrating gives

12(z1+z2+ln⁑(z+1+z2))+12z2=ln⁑x+c,\tfrac{1}{2}\Big(z\sqrt{1 + z^2} + \ln\big(z + \sqrt{1 + z^2}\big)\Big) + \tfrac{1}{2}z^2 = \ln x + c,

with z=y/xz = y/x put back at the end.

Problem 3 Β· Solve It

Given: yβ€²=x2+y2xyy' = \dfrac{x^2 + y^2}{xy} with x>0x > 0. Find the general solution.

βœ… Correct! F(z)βˆ’z=1zF(z) - z = \dfrac{1}{z}, so z dz=dxxz\,dz = \dfrac{dx}{x}, 12z2=ln⁑x+c\tfrac{1}{2}z^2 = \ln x + c, and putting back z=y/xz = y/x gives y2=x2(2ln⁑x+C)y^2 = x^2(2\ln x + C).
❌ Not quite. That comes from xzβ€²=F(z)x z' = F(z), the substitution without its +z+z, and it solves yβ€²=x2+2y2xyy' = \dfrac{x^2 + 2y^2}{xy} instead. With yβ€²=zβ€²x+zy' = z'x + z the right side is F(z)βˆ’z=1zF(z) - z = \dfrac{1}{z}.
❌ Not quite. Integrating z dzz\,dz gives 12z2\tfrac{1}{2}z^2, so z2=2ln⁑x+2cz^2 = 2\ln x + 2c: the 22 multiplies ln⁑x\ln x and cannot be absorbed into the constant.
❌ Not quite. 12z2=ln⁑x+c\tfrac{1}{2}z^2 = \ln x + c is still in zz. Putting back z=y/xz = y/x gives y2x2=2ln⁑x+C\dfrac{y^2}{x^2} = 2\ln x + C, so the factor x2x^2 belongs on the right.
Show solution

Step 1: divide top and bottom by x2x^2:

F(z)=1+z2z=1z+zF(z) = \frac{1 + z^2}{z} = \frac{1}{z} + z

Step 2: substitute y=zxy = zx, yβ€²=zβ€²x+zy' = z'x + z:

zβ€²x+z=1z+zβ€…β€ŠβŸΉβ€…β€Šx dzdx=1zz'x + z = \frac{1}{z} + z \;\Longrightarrow\; x\,\frac{dz}{dx} = \frac{1}{z}

Step 3: separate and integrate:

z dz=dxxβ€…β€ŠβŸΉβ€…β€Š12z2=ln⁑x+cz\,dz = \frac{dx}{x} \;\Longrightarrow\; \tfrac{1}{2}z^2 = \ln x + c

Step 4: put back z=y/xz = y/x, with C=2cC = 2c:

y2x2=2ln⁑x+Cβ€…β€ŠβŸΉβ€…β€Šy2=x2(2ln⁑x+C)\frac{y^2}{x^2} = 2\ln x + C \;\Longrightarrow\; y^2 = x^2\big(2\ln x + C\big)

Check: 2yyβ€²=2x(2ln⁑x+C)+2x=2y2x+2x2yy' = 2x(2\ln x + C) + 2x = \dfrac{2y^2}{x} + 2x, so yβ€²=yx+xy=x2+y2xyy' = \dfrac{y}{x} + \dfrac{x}{y} = \dfrac{x^2 + y^2}{xy}. No line is lost, because F(z)βˆ’z=1zF(z) - z = \dfrac{1}{z} is never zero.

Problem 4 Β· Lines the Division Loses

Given: yβ€²=y2+2xyx2y' = \dfrac{y^2 + 2xy}{x^2}. Which straight lines y=z0xy = z_0 x are solutions?

βœ… Correct! A line y=z0xy = z_0 x has slope z0z_0, so it solves the equation exactly when F(z0)=z0F(z_0) = z_0: z02+2z0=z0z_0^2 + 2z_0 = z_0, that is z0(z0+1)=0z_0(z_0 + 1) = 0.
❌ Not quite. The condition z02+z0=0z_0^2 + z_0 = 0 factors as z0(z0+1)=0z_0(z_0 + 1) = 0, so z0=βˆ’1z_0 = -1 is a root too, and y=βˆ’xy = -x checks: yβ€²=βˆ’1y' = -1 and x2βˆ’2x2x2=βˆ’1\dfrac{x^2 - 2x^2}{x^2} = -1.
❌ Not quite. That solves F(z0)=0F(z_0) = 0, which would make the slope zero. A line y=z0xy = z_0 x has slope z0z_0, so the condition is F(z0)=z0F(z_0) = z_0; on y=βˆ’2xy = -2x the right side is 00 but the slope is βˆ’2-2.
❌ Not quite. On a line y=z0xy = z_0 x the right side of a homogeneous equation is the constant F(z0)F(z_0), so the line is a solution whenever that constant equals its slope z0z_0, nonlinear or not.
Show solution

Divide top and bottom by x2x^2: yβ€²=(y/x)2+2(y/x)y' = (y/x)^2 + 2(y/x), so F(z)=z2+2zF(z) = z^2 + 2z. On the line y=z0xy = z_0 x both sides are constant, yβ€²=z0y' = z_0 and F(y/x)=F(z0)F(y/x) = F(z_0):

F(z0)=z0β€…β€ŠβŸΊβ€…β€Šz02+z0=0β€…β€ŠβŸΊβ€…β€Šz0=0Β orΒ z0=βˆ’1F(z_0) = z_0 \iff z_0^2 + z_0 = 0 \iff z_0 = 0 \ \text{or}\ z_0 = -1

So the lines are y=0y = 0 and y=βˆ’xy = -x. They are exactly the zeros of F(z)βˆ’z=z(z+1)F(z) - z = z(z + 1), the factor the separation step divides out:

dzz(z+1)=dxxβ€…β€ŠβŸΉβ€…β€Šln⁑∣zz+1∣=ln⁑∣x∣+cβ€…β€ŠβŸΉβ€…β€Šy=Kx21βˆ’Kx\frac{dz}{z(z + 1)} = \frac{dx}{x} \;\Longrightarrow\; \ln\left|\frac{z}{z + 1}\right| = \ln|x| + c \;\Longrightarrow\; y = \frac{Kx^2}{1 - Kx}

K=0K = 0 happens to bring back y=0y = 0, but no value of KK gives y=βˆ’xy = -x: that solution survives only because it was found before dividing.

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